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Untitled - Aerobib - Universidad Politécnica de Madrid

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6.15. FLAME PROPAGATION IN HYDROGEN-BROMINE MIXTURES 187<br />

6.15 Flame propagation in Hydrogen-Bromine mixtures<br />

The present example contains a calculation of the velocity of the hydrogen-bromine<br />

flame performed with a variation of the method <strong>de</strong>veloped by von Kármán and Penner<br />

[40]. The method presented here differs from earlier calculations because the<br />

influence of dissociation of bromine on the flame velocity is evaluated properly. Von<br />

Kármán and Penner inclu<strong>de</strong>d the influence of the atoms of bromine on the reaction<br />

rate but when calculating the distribution of the mole fraction of Br 2 , H 2 and HBr,<br />

they neglected the mole fraction of Br atoms. However, for temperatures close to the<br />

maximum flame temperature the dissociation of Br 2 reduces substantially the value<br />

for the mole fraction of Br 2 , which has an important influence on the flame velocity.<br />

Hence it seemed <strong>de</strong>sirable to compute the burning velocity correctly, especially<br />

in hydrogen-rich flames where the influence of dissociation is most important. Von<br />

Kármán and Penner also neglect the influence of the energy of dissociation of Br 2 ,<br />

which should be taken into account since it may be of the same or<strong>de</strong>r of magnitu<strong>de</strong> as<br />

the energy transferred by convection through the flame.<br />

In the following, a method is <strong>de</strong>veloped for the correct calculation of the mole<br />

fraction of Br 2 and of the influence of its dissociation energy on the velocity of the<br />

flame, within the limitations of the steady-state assumption for the distribution of<br />

bromine and hydrogen atoms. This method will be applied to computation for the<br />

four hydrogen-rich flames previously consi<strong>de</strong>red by von Kármán and Penner. The results<br />

are compared with those obtained by these authors and are shown to differ by not<br />

more than 25% even for the hottest flame.<br />

A <strong>de</strong>tailed study of the structure of the flame is also presented. It will be shown<br />

that dissociation of Br 2 reduces the flame velocity because of a <strong>de</strong>crease in the number<br />

of molecules of bromine which exist near the hot flame boundary. On the other hand,<br />

it will be seen that the influence of the dissociation energy can be neglected if thermal<br />

convection is ignored because these two effects tend to cancel.<br />

The procedure <strong>de</strong>veloped here follows closely the work performed in Ref. [41]<br />

and could also be useful for computations on other types of flames.<br />

Flame Equations<br />

Since there are only five different chemical components, namely, HBr, Br 2 , H 2 , Br<br />

and H, the unknowns are:<br />

1) Five flux fractions, ε i .

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